topic 9 Flashcards
(14 cards)
electrons behave like a tiny bar magnet
due to intrinsic angular momentum of an electron (s)
- has magnetic moment (us)
- must be quantised
the orbital angular momentum of an electron with l>0 leads to
a second source of atomic magnetic moment ul
- magnetic moment vectors oriented in opposite direction to angular momentum vectors from which they stem from
- must be quantised (values that make up equation are quantised)
spin - orbit coupling
- magnetic interaction between quantised spin and orbital magnetic moments of an electron
- leads to total angular momentum J
- internal interaction = splitting
Zeeman effect
- external interaction between an atom and an applied magnetic field that further spilts the energy of the levels into individual states
in an applied magnetic field, B, energy of the magnetic moment associated with the total angular moment, uj, of an electron
changes
- change in energy depend on the relative orientation of the magnetic moment (quantised by Mj) and the direction of the applied field
- Zeeman effect
hands rules involving spin - orbit coupling
- for a sub shell less than half full, lowest J = ground level
- for a sub shell more than half full, highest J = ground level
- for an exactly filled half - sub shell there is no spin - orbit coupling in ground state due to rules of maximum multiplicity
how is the hole formalism (configuration of holes and electrons give rise to the same terms) effected by spin - orbit coupling
- the splitting term is reversed due to hunds 3rd rule and so pairs of electron configurations have different ground state level
energy of level 2s+1L (term)
E_L,S,J = hcA( J(J+1) - L(L+1) - S(S+1)/ all divided by 2)
- A is spin - orbit coupling constant (cm^-1)
coupling constant A
- increases with atomic number and scales roughly as A proportion to Z^4
- less than Half filled sub shell A>0 Such that E(J) increases as J increases
- more than half filled sub shell A<0 such that E(J) decrease as J increases
lande interval rule
- for levels of the same term, the values of L and S are the same
- thus the energy spacing between levels J and J + 1
= hcA (J + 1)
selection rules
- change in J = 0, +/- 1
- change in S = 0
- change in L = 0, +/- 1 (provided change in l = +/- 1)
- chang in n = no restrictions
- change in Mj states = 0, +/- 1
spin - orbit coupling spectral line splitting
- alkali metals where p electron of an electronically excited state relaxes to a lower s orbital, spin orbit coupling gives rise to important spectral feature
- look at strong line at 589 nm under high resolution, see doublet
- due to spin - orbit coupling
- down the alkali metal group the splitting increases with spin - orbit coupling constant ( A proportional to Z^4)
- doublet because line splitting from 2p3/2 to 2S1/2 and 2P1/2 to 2S1/2
Zeeman effect equation
- E = -total angular momentum (uj) x applied magnetic field (B) = - modulus uj x modulus B x cos(theta)
the stronger the applied field
the stronger the spectral line splitting